Protective passivation layer for magnetic tunnel junctions
A magnetic device for magnetic random access memory (MRAM), spin torque MRAM, or spin torque oscillator technology is disclosed wherein a magnetic tunnel junction (MTJ) with a sidewall is formed between a bottom electrode and a top electrode. A passivation layer that is a single layer or multilayer comprising one of B, C, or Ge, or an alloy thereof wherein the B, C, and Ge content, respectively, is at least 10 atomic % is formed on the MTJ sidewall to protect the MTJ from reactive species during subsequent processing including deposition of a dielectric layer that electrically isolates the MTJ from adjacent MTJs, and during annealing steps around 400° C. in CMOS fabrication. The single layer is about 3 to 10 Angstroms thick and may be an oxide or nitride of B, C, or Ge. The passivation layer is preferably amorphous to prevent diffusion of reactive oxygen or nitrogen species.
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The present application is a divisional application of U.S. application Ser. No. 15/463,113, entitled “Protective Passivation Layer for Magnetic Tunnel Junctions,” filed Mar. 20, 2017, which application is herein incorporated by reference in its entirety.
RELATED PATENT APPLICATIONThis application is related to the following: U.S. Pat. No. 9,230,571; assigned to a common assignee, and herein incorporated by reference in its entirety.
TECHNICAL FIELDThe present disclosure relates to magnetic tunnel junctions (MTJs) in magnetic random access memory (MRAM), spin-torque MRAM, and other spintronic devices, and in particular to protecting MTJ sidewalls during processing steps including the deposition of an insulating dielectric layer that separates adjacent MTJs, and during high temperature annealing around 400° C. that is common in Complementary Metal Oxide Semiconductor (CMOS) fabrication.
BACKGROUNDA MTJ is a key component in MRAM, spin-torque MRAM, and other spintronic devices and comprises a stack with a tunnel barrier layer such as a metal oxide formed between two magnetic layers that provides a tunneling magnetoresistance (TMR) effect. One of the magnetic layers is a free layer and serves as a sensing layer by switching the direction of its magnetic moment in response to external fields while the second magnetic layer has a magnetic moment that is fixed and functions as a reference layer. The electrical resistance through the tunnel barrier layer (insulator layer) varies with the relative orientation of the free layer moment compared with the reference layer moment and thereby provides an electrical signal that is representative of a magnetic state in the free layer. In a MRAM, the MTJ is formed between a top conductor and bottom conductor. When a current is passed through the MTJ, a lower resistance is detected when the magnetization directions of the free and reference layers are in a parallel state and a higher resistance is noted when they are in an anti-parallel state. Since MTJ elements are often integrated in CMOS devices, the MTJ must be able to withstand annealing temperatures around 400° C. for about 30 minutes that are commonly applied to improve the quality of the CMOS units for semiconductor purposes.
MTJ elements wherein the free layer (FL) and reference layer (RL) have perpendicular magnetic anisotropy (PMA) are preferred over their counterparts that employ in-plane anisotropy because a PMA-MTJ has an advantage in a lower writing current for the same thermal stability, and better scalability. In MTJs with PMA, the FL has two preferred magnetization orientations that are perpendicular to the physical plane of the layer. Without external influence, the magnetic moment of the free layer will align to one of the preferred two directions, representing information “1” or “0” in the binary system. For memory applications, the FL magnetization direction is expected to be maintained during a read operation and idle, but change to the opposite direction during a write operation if the new information to store differs from its current memory state. CoFeB or the like is commonly used as the FL and RL, and MgO is preferred as the tunnel barrier to generate PMA along the RL/MgO and MgO/FL interfaces in a RL/MgO/FL stack.
Spin-torque (STT)-MRAM based technologies are desirable for nonvolatile memory applications. However, realizing low critical dimensions below 100 nm that match those found in Dynamic Random Access Memory (DRAM) is a challenge. MTJs are highly susceptible to sidewall damage, both chemical and physical, induced by etching and deposition processes, and exacerbated by the CMOS process requirement of annealing at 400° C.
During fabrication of a conventional STT-MRAM device where a dielectric layer is deposited on MTJ sidewalls in order to insulate the MTJ from adjacent MTJ devices in the STT-MRAM array, damage frequently occurs to the MTJ sidewalls. Damage may result from oxygen diffusion through a MTJ sidewall during an oxide dielectric layer deposition, for example, and thereby oxidize a significant portion of the MTJ. In some cases, metal from a MTJ capping layer may be redeposited on MTJ sidewalls to cause shunting around the tunnel barrier layer, or electrical short circuits. As a result, there is a reduction in device performance, substantial non-uniformity between bits that translates into an undesirable larger distribution of key metrics, and lower device yields. Reducing sidewall damage is especially important at the CoFeB/MgO (RL/tunnel barrier and tunnel barrier/FL) interfaces that generate interfacial PMA. Furthermore, the delicate nature of the MgO tunnel barrier layer is well known to have poor corrosion properties and readily degrades when exposed to atmosphere during deposition of the insulating dielectric layer.
Although methods are available to remove sidewall damage caused by ion bombardment, and by exposure to atmosphere during dielectric layer deposition, the methods are generally time consuming and costly. Moreover, some sidewall damage may be too extensive to repair. There is a need to prevent MTJ sidewall damage by providing a means of protecting a MTJ element during subsequent process steps in memory device fabrication.
SUMMARYOne objective of the present disclosure is to substantially improve the resistance of a MTJ to sidewall damage during etching, deposition, and annealing processes in memory device fabrication.
A second objective of the present disclosure is to provide a method of delivering the MTJ integrity improvement according to the first objective that is compatible with back end of line (BEOL) CMOS processes.
According to one embodiment of the present disclosure, these objectives are achieved by depositing a protective passivation layer on a MTJ sidewall during fabrication of a memory device. The passivation layer may be RF magnetron sputtered, or formed by an atomic layer deposition (ALD) technique, chemical vapor deposition (CVD) method, or a physical vapor deposition (PVD) method. According to one preferred embodiment, the passivation layer is a single layer of B, C, or Ge that is sputter deposited with a RF power from about 100 to 1000 Watts in the absence of a reactive species such as nitrogen containing and oxygen containing gases and plasmas. The passivation layer has a thickness of at least 3 Angstroms to enable a continuous coating. Preferably, the passivation layer is amorphous and not crystalline to prevent diffusion of reactive materials between crystals in a lattice.
In another embodiment, an oxidation process such as a natural oxidation (NOX) is employed to partially or totally oxidize a B layer to BO, a C layer to CO, or a Ge layer to GeO passivation layer. Alternatively, a B, C, or Ge layer is deposited in a first step, and is then exposed to a nitridation or oxynitridation process to form a BN, CN, GeN, BON, CON, or GeON passivation layer, respectively, having a non-stoichiometric or stoichiometric N content. Depending on the conditions employed in the aforementioned oxidation process, a B/BO bilayer, C/CO bilayer, or Ge/GeO bilayer may be formed. In another embodiment, a B, C, or Ge passivation layer reacts with oxygen species during deposition of a dielectric layer and is partially or totally oxidized to a BO, CO, or GeO passivation layer.
In another embodiment, a passivation layer that comprises an alloy may be fabricated by a two step deposition sequence. In particular, an alloy with a BX, CX, or GeX composition is formed by a first step of depositing a B, C, or Ge layer, and then a second step of depositing an X element where X is one of B, C, Ge, Si, Al, P, Ga, In, TI, Mg, Hf, Zr, Nb, V, Ti, Cr, Mo, W, Sr, and Zn, and where X is unequal to the other element in the alloy. In other words, the initially deposited B, C, or Ge layer serves as a sacrificial material and is completely resputtered during the X deposition, and combines with the X element to form an alloy. Preferably, B in BX, C in CX, and Ge in GeX has a content of at least 10 atomic %.
According to another embodiment, the two step deposition previously described is followed. However, during the second step involving X deposition, only an upper (outer) portion of the B, C, or Ge first passivation layer is resputtered to form a second passivation layer comprised of BX, CX, or GeX, respectively, thereby generating a B/BX, C/CX, or Ge/GeX bilayer structure as a composite passivation layer. Here, the duration of the second deposition is shortened, or the process conditions during the X deposition may be adjusted to employ a weaker RF power, for example, to prevent the entire B, C, or Ge layer from being resputtered.
A two step deposition process is advantageous in that the first step of depositing a B, C, or Ge layer is effective in protecting MTJ sidewalls from reactive species such as oxygen. The second step of depositing an X material to form either a bilayer or a single alloy layer is primarily relied on to prevent damage to MTJ sidewalls from high-energy ions during subsequent processes including dielectric layer deposition.
In yet another embodiment where two deposition steps are used to form a passivation layer, one or both of oxygen and nitrogen may be included in the second deposition step. Thus, the present disclosure anticipates formation of a bilayer such as B/BXO, C/CXO, Ge/GeXO, B/BXN, C/CXN, Ge/GeXN, B/BXON, C/CXON, or Ge/GeXON when depositing an X layer on a B, C, or Ge layer in the presence of a reactive species that comprises one or both of an oxygen species and a nitrogen species. Furthermore, the oxide, nitride, and oxynitride layers may be a composite such that a BXO layer, for example, comprises BO and BX, BXN comprises BN and BX, and BXON comprises BON and BX, respectively.
In the completed memory structure that may be a MRAM, STT-MRAM, or spin torque oscillator (STO), there is an array of MTJ elements formed in a plurality of rows and columns on a substrate. In a MRAM or STT-MRAM application, the substrate comprises a bottom electrode layer wherein there is a plurality of conductive lines so that a bottom surface of each MTJ contacts a conductive line. Each MTJ has a sidewall that is protectively covered by a passivation layer according to an embodiment described herein. Moreover, there is a dielectric layer that contacts a top surface of the passivation layer and fills the spaces between adjacent MTJ elements. The dielectric layer may be comprised of one or more oxides, nitrides, oxynitrides, or carbides used in the art for electrical insulation purposes, and may have a top surface that is coplanar with a top surface of the MTJ. A top electrode layer comprised of a plurality of conductive lines is formed on the array of MTJ elements such that each MTJ is formed between a bottom electrode and a top electrode.
In a STO device, the substrate may be a main pole layer that serves as a bottom electrode, and the top electrode may be a trailing shield, for example. A passivation layer is formed on a side of the STO stack of layers that faces away from an air-bearing surface (ABS).
The present disclosure relates to improved structural integrity in MTJ elements, especially during processes that involve deposition of dielectric layers between MTJ sidewalls, and exposure to high temperatures around 400° C. The MTJ elements may be formed in a variety of memory devices including but not limited to MRAM, spin-torque MRAM, and other spintronic devices such as a spin torque oscillator (STO). In the drawings, a thickness of a layer is in the z-axis direction, a width is in the x-axis direction, and a length is in the y-axis direction. The terms “dielectric” and “insulation” may be used interchangeably.
As mentioned previously, many memory devices are now incorporated into CMOS platforms in order to provide higher performance. However, we observe substantially higher defects and degraded device performance when dielectric layers are deposited directly on MTJ sidewalls by conventional methods, and the resulting device is annealed at temperatures around 400° C. that are required in CMOS processing. Thus, we were motivated to implement a means of protecting MTJ elements to provide higher performance and yields in memory applications.
Referring to
It should be understood that typically millions of MTJs are aligned in rows and columns in a memory array on a substrate, and each MTJ is formed between a bottom electrode and a top electrode. However, the number of MTJs shown in
Preferably, passivation layer 12 has a uniform thickness, and contacts not only MTJ sidewalls 11s1 and 11s2, and other MTJ sidewalls that are not depicted, but also adjoins portions of top surfaces of bottom electrodes such as top surface 10t of bottom electrode 10a that are not covered by MTJs. According to one aspect, the passivation layer is non-magnetic and is a single layer with a thickness of at least 3 Angstroms to enable a continuous coating. In a preferred embodiment, the passivation layer is amorphous and not crystalline to prevent diffusion of reactive materials between crystals in a lattice, and may be a single layer of B, C, or Ge. A carbon passivation layer may have a diamond-like structure or a high degree of sp3 bonding that is deposited by a CVD or PVD method. We have discovered that the maximum advantage of a more uniform coercivity (Hc) over a range of MTJ sizes is minimized for a B passivation layer thickness of about 5 Angstroms, and decreases somewhat when the thickness is increased to 10 Angstroms or more. Furthermore, a key feature of all passivation layers disclosed herein is a capability to protect MTJ sidewalls from attack by reactive species during processes including deposition of a dielectric layer between MTJ elements.
The present disclosure also encompasses a method of forming a single passivation layer on the MTJ sidewalls. First, a method of fabricating a plurality of MTJs is described. In
A photoresist layer is formed on the MTJ stack of layers and is patterned by a well known photolithography technique to give a plurality of islands including photoresist islands 30a, 30b each having a width w. Subsequently, a conventional reactive ion etch (RIE) or ion beam etch (IBE) process is performed to remove regions of the MTJ stack of layers that are not protected by a photoresist island. Note that the photolithography process yields an array of photoresist islands laid out in rows and columns such that each island serves as an etch mask, and the RIE or IBE process generates a MTJ below each etch mask. Thus, MTJ 11a and MTJ 11b are formed with sidewalls 11s1 and 11s2, respectively, below islands 30a and 30b, and there are openings 50 on each side of the MTJs that expose portions of bottom electrode top surface 10t. In the exemplary embodiment, the RIE or IBE process forms non-vertical sidewalls 11s1 and 11s2 such that a bottom of each MTJ at top surface 10t has a greater width than w. However, depending on the etch conditions, substantially vertical MTJ sidewalls may be produced.
Referring to
Preferably, the passivation layer is conformally deposited with a thickness on sidewalls 11s1 and 11s2 that is essentially equivalent to a thickness on bottom electrode top surface 10t. Although it is difficult to measure thin passivation layer thicknesses on the order of 5-10 Angstroms during device fabrication, an independent experiment may be performed where a substantially thicker film of B, for example, is deposited on a planar (non-product) substrate during a time period “d”. Once the B film thickness “t” is measured by a transmission electron microscope (TEM) technique, a deposition rate “t/d” in Angstroms per minute is determined for the deposition process. Then, the deposition rate is used to calculate a deposition time substantially less than “d” to yield a thin passivation layer about 5-10 Angstroms thick on substrates comprising MTJs 11a, 11b.
Referring to
According to one embodiment shown in
Returning to
It should be understood that passivation layer 12 in
According to another single layer embodiment depicted in
The present disclosure also encompasses an embodiment where a BN, BO, BON, CN, CO, CON, GeN, GeO, or GeON target is used to deposit a single passivation layer 12x on MTJ sidewalls 11s1, 11s2 as depicted in
As shown in
According to another embodiment of the present disclosure shown in
Another single passivation layer embodiment is shown in
Referring to
Another embodiment of the present disclosure is illustrated in
As shown in
As indicated in
Referring to
Referring to
Referring to
In
During a write process, magnetic flux 8 passes through the ABS 33-33 and transits the magnetic medium 7 and soft underlayer 6 and flux 8a re-enters the write head through trailing shield 18. Under a gap field 8b of several thousand Oe and a dc bias across the STO, the write process is assisted by a spin polarized current passing from the SP layer 42 to the OL 44 with sufficient magnitude (critical current density) to cause a large angle oscillation 47 with a certain amplitude and frequency in the OL that imparts a rf field 49 on medium bit 9. The combined effect of the rf field and magnetic field 8 enables the magnetization 5 in the bit to be switched with a lower magnetic field than when only magnetic field 8 is applied.
The STO device 40 is considered to be a MTJ where the SP layer 42 serves as a reference layer, the non-magnetic spacer 43 is a tunnel barrier, and OL layer 44 is effectively a free layer. The composition of layers 41-45 is described in detail in related U.S. Pat. No. 9,230,571. A key feature of the present disclosure is that passivation layer 12 is formed on a trailing side 17t of the main pole and on a sidewall 40s of STO 40 thereby protecting the sidewall during deposition of dielectric layer 13 that is formed between main pole layer 17 and trailing shield 18. As a result, the STO device retains structural integrity during subsequent fabrication steps unlike the prior art where the STO sidewall is susceptible to damage by reactive gases used in the deposition of the dielectric layer.
Referring to
Results in
In
Referring to
The one or more additional deposition steps and minimal cost required to form a protective passivation layer described herein is considered insignificant when compared with the substantial cost involved in attempting to repair a POR MTJ that was damaged during dielectric layer deposition, and the waste (lower yield) associated with POR MTJs that are damaged beyond repair. The protective passivation layers of the present disclosure may be deposited by employing conventional tools and materials used in the art.
While this disclosure has been particularly shown and described with reference to, the preferred embodiment thereof, it will be understood by those skilled in the art that various changes in form and details may be made without departing from the spirit and scope of this disclosure.
Claims
1. A method, comprising:
- forming a magnetic tunnel junction (MTJ) on a top surface of a substrate, wherein the MTJ has a MTJ top surface and MTJ sidewalls that extends from the MTJ top surface to the top surface of the substrate;
- depositing a passivation layer that is non-magnetic, the passivation layer including one or more layers selected from the group consisting of a BSi-containing layer, a BX alloy-containing layer, a CX alloy-containing layer, a GeSi-containing layer, and a GeX alloy-containing layer, wherein X is one of B, C, Ge, Al, P, Ga, In, Tl, Mg, Hf, Zr, Nb, V, Ti, Cr, Mo, W, Sr, and Zn, and wherein the passivation layer is deposited on exposed portions of the top surface of the substrate, the MTJ sidewalls, and the MTJ top surface;
- subjecting the passivation layer to an oxidation, nitridation, or oxynitridation process such that a first layer of the one or more layers of the passivation layer is entirely transformed to an oxide, nitride, or oxynitride, respectively, of the BSi-containing layer, the BX alloy-containing layer, the CX alloy-containing layer, the GeSi-containing layer, or the GeX alloy-containing layer; and
- depositing a dielectric layer on the passivation layer, wherein the dielectric layer electrically isolates the MTJ from another MTJ.
2. The method of claim 1, further comprising:
- planarizing the dielectric layer such that a top surface of the dielectric layer is substantially aligned with the MTJ top surface; and
- performing an anneal process at a temperature of about 400° C.
3. The method of claim 1, wherein the substrate is a bottom electrode in a MRAM or spin torque MRAM.
4. The method of claim 1, wherein the substrate is a main pole layer in a spin torque oscillator.
5. The method of claim 1, wherein at least one layer of the one or more layers of the passivation layer has a thickness from about 3 Angstroms to about 10 Angstroms.
6. The method of claim 1, wherein a concentration of X in the BX alloy of the BX alloy-containing layer, the CX alloy of the CX alloy-containing layer, or the GeX alloy of the GeX alloy-containing layer is at least 10 atomic %.
7. The method of claim 1, wherein the subjecting the passivation layer to the oxidation, nitridation, or oxynitridation process subjects the first layer of the one or more layers of the passivation layer to the oxidation process before depositing the dielectric layer to form the oxide of the BSi-containing layer, the BX alloy-containing layer, the CX alloy-containing layer, the GeSi-containing layer, or the GeX alloy-containing layer.
8. The method of claim 7, wherein the oxidation process includes a natural oxidation with an oxygen flow rate from about 1 standard cubic centimeters per minute (sccm) to about 10 sccm for a period from about 10 seconds to about 600 seconds.
9. The method of claim 1, wherein the subjecting the passivation layer to the oxidation, nitridation, or oxynitridation process subjects the first layer of the one or more layers of the passivation layer to the nitridation process before depositing the dielectric layer to form the nitride of the BSi-containing layer, the BX alloy-containing layer, the CX alloy-containing layer, the GeSi-containing layer, or the GeX alloy-containing layer.
10. A method, comprising:
- forming a plurality of magnetic tunnel junctions (MTJs) on a top surface of a substrate, wherein each of the plurality of MTJs has a MTJ top surface and a MTJ sidewall that extends from the MTJ top surface to the top surface of the substrate;
- forming a first passivation layer on exposed portions of the top surface of the substrate, the MTJ sidewalls, and the MTJ top surfaces, the first passivation layer being a boron (B)-containing layer, a carbon (C)-containing layer, or a germanium (Ge)-containing layer; and
- depositing Si or an X element on the first passivation layer such that an upper portion of the first passivation layer is resputtered to form a second passivation layer, wherein X is one of B, C, Ge, Al, P, Ga, In, Tl, Mg, Hf, Zr, Nb, V, Ti, Cr, Mo, W, Sr, and Zn, and wherein the second passivation layer is one of a BSi-containing layer, a BX alloy-containing layer, a CX alloy-containing layer, a GeSi-containing layer, or a GeX alloy-containing layer.
11. The method of claim 10, further comprising subjecting the second passivation layer to an oxidation, nitridation, or oxynitridation process such that an upper portion of the second passivation layer is converted to a third passivation layer that is an oxide, nitride, or oxynitride of the second passivation layer.
12. The method of claim 10, further comprised of subjecting the second passivation layer to an oxidation, nitridation, or oxynitridation process such that an entirety of the second passivation layer is converted to an oxide, nitride, or oxynitride of the BSi-containing layer, the BX alloy-containing layer, the CX alloy-containing layer, the GeSi-containing layer, or the GeX alloy-containing layer.
13. The method of claim 10, wherein forming the first passivation layer includes a sputter deposition process with a radio frequency (RF) power from about 100 Watts to about 1000 Watts, and a chamber pressure from about 0.05 mTorr to about 20 mTorr.
14. A method, comprising:
- forming a magnetic tunnel junction (MTJ) on a top surface of a substrate, wherein the MTJ has MTJ sidewalls that extends from a MTJ top surface to the top surface of the substrate;
- forming a passivation layer having one or more layers on the MTJ sidewalls, the MTJ top surface, and exposed portions of the top surface of the substrate in an absence of a reactive oxygen species or a reactive nitrogen species, wherein a first layer of the one or more layers of the passivation layer has a thickness from about 3 Angstroms to about 10 Angstroms; and
- forming a dielectric layer on the passivation layer.
15. The method of claim 14, wherein the one or more layers of the passivation layer is selected from the group consisting of a boron (B)-containing layer, a BSi-containing layer, a BX alloy-containing layer, a carbon (C)-containing layer, a CX alloy-containing layer, a germanium (Ge)-containing layer, a GeSi-containing layer, and a GeX alloy-containing layer, wherein X is one of B, C, Ge, Al, P, Ga, In, Tl, Mg, Hf, Zr, Nb, V, Ti, Cr, Mo, W, Sr, and Zn.
16. The method of claim 14, wherein the one or more layers of the passivation layer is selected from the group consisting of a BN-containing layer, a BO-containing layer, a BON-containing layer, a CN-containing layer, a CO-containing layer, a CON-containing layer, a GeN-containing layer, a GeO-containing layer, or a GeON-containing layer.
17. The method of claim 14, wherein the first passivation layer is selected from the group consisting of a boron (B)-containing layer, a carbon (C)-containing layer, and a germanium (Ge)-containing layer.
18. The method of claim 14, subjecting the first passivation layer to an oxidation, nitridation, or oxynitridation process such that only a portion of the first passivation layer is transformed to an oxide, nitride, or oxynitride, respectively, of the boron (B)-containing layer, the carbon (C)-containing layer or the germanium (Ge)-containing layer.
19. The method of claim 14, wherein the one or more layers of the passivation layer is selected from the group consisting of a BX alloy-containing layer, CX alloy-containing layer and a GeX alloy-containing layer, and
- wherein X is one of B, C, Ge, Al, P, Ga, In, Tl, Mg, Hf, Zr, Nb, V, Ti, Cr, Mo, W, Sr, and Zn.
20. The method of claim 14, further comprising directing Si or an X element at the first passivation layer such that an upper portion of the first passivation layer is resputtered to form a second passivation layer, wherein X is one of B, C, Ge, Al, P, Ga, In, Tl, Mg, Hf, Zr, Nb, V, Ti, Cr, Mo, W, Sr, and Zn.
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Type: Grant
Filed: Oct 7, 2019
Date of Patent: Jun 1, 2021
Patent Publication Number: 20200035912
Assignee: TAIWAN SEMICONDUCTOR MANUFACTURING COMPANY, LTD. (Hsinchu)
Inventors: Jodi Mari Iwata (San Carlos, CA), Guenole Jan (San Jose, CA), Ru-Ying Tong (Los Gatos, CA)
Primary Examiner: Sonya McCall-Shepard
Application Number: 16/594,339
International Classification: H01L 43/08 (20060101); H01L 21/02 (20060101); H01L 43/12 (20060101); H01L 27/22 (20060101); H01F 10/32 (20060101); H03B 15/00 (20060101); H01L 43/02 (20060101);